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Sound Power Intensity Pressure

Reference data and engineering information about sound power intensity pressure for acoustics applications.

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Overview

Engineering reference data for Sound Power Intensity Pressure in acoustics.

Key Formulas

Speed of Sound

c=γRTc = \sqrt{\gamma R T}

Speed of sound in an ideal gas.

Sound Level

L=10log10(I/I0)L = 10 \log_{10}(I/I_0)

Decibel level.

Wavelength

λ=c/f\lambda = c / f

Wavelength = speed / frequency.

Variables

SymbolDescriptionUnit
ccSpeed of soundm/s
LLSound leveldB
λ\lambdaWavelengthm
ffFrequencyHz

Additional Relationships and Properties

Sound Intensity and Pressure Relationship

The acoustic intensity II is related to the root-mean-square (rms) sound pressure pp and the characteristic acoustic impedance of the medium ρc\rho c (where ρ\rho is density and cc is speed of sound) by: I=p2ρcI = \frac{p^2}{\rho c} This relationship is crucial for connecting measurements made with pressure microphones to intensity calculations.

Inverse Square Law

For a point source radiating sound power WW uniformly into a free field, the sound intensity II decreases with the square of the distance rr from the source: I=W4πr2I = \frac{W}{4\pi r^2} This demonstrates that the Sound Intensity Level LIL_I decreases by approximately 6 dB each time the distance from a point source is doubled.

Practical Note on Sound Pressure Level

A key practical consequence derived from formula (4) is that a doubling of sound pressure (p2=2p1p_2 = 2p_1) results in a 6 dB increase in Sound Pressure Level: ΔLp=20log10(2)6.02 dB\Delta L_p = 20 \log_{10}(2) \approx 6.02 \ \text{dB} This "6-dB rule" is a fundamental reference for assessing changes in loudness perception and acoustic exposure.

References